A DENSITY-FUNCTIONAL STUDY ON THE ORIGIN OF THE PROPAGATION BARRIER IN THE HOMOGENEOUS ETHYLENE POLYMERIZATION WITH KAMINSKY-TYPE CATALYSTS

Citation
Jcw. Lohrenz et al., A DENSITY-FUNCTIONAL STUDY ON THE ORIGIN OF THE PROPAGATION BARRIER IN THE HOMOGENEOUS ETHYLENE POLYMERIZATION WITH KAMINSKY-TYPE CATALYSTS, Journal of the American Chemical Society, 117(51), 1995, pp. 12793-12800
Citations number
60
Categorie Soggetti
Chemistry
ISSN journal
00027863
Volume
117
Issue
51
Year of publication
1995
Pages
12793 - 12800
Database
ISI
SICI code
0002-7863(1995)117:51<12793:ADSOTO>2.0.ZU;2-R
Abstract
The reaction of ethylene with Cp(2)Zr(+)-Et has been studied with nonl ocal density functional theory (DFT). Comparison of four different cha in orientations in Cp(2)Zr(+)-Bu reveals the high stability of a beta- agostic resting state as compared to delta- (+30.9 kJ/mol), gamma-(+26 .9 kJ/mol), and alpha-agostic (+46.8 kJ/mol) structures. Thus the beta -agostic Cp(2)Zr(+)-Et was chosen as the model for the resting state. A beta-agostic pi-complex is formed in an exothermic reaction (Delta H = -37.1 kJ/mol). Before insertion can take place, rotation around Zr- C-alpha has to take place in order to form an alpha-agostic intermedia te. The electronic barrier for this process amounts to 14.0 kJ/mol and is compensated by a positive entropy of activation (Delta S double da gger = +5.5 J/(mol . K)), a negative change in zero-point energy (Delt a H-0 = -10.4 kJ/mol), and vibrational energy (Delta H-vib = +2.11 kJ/ mol), giving rise to a negligible free energy of activation (Delta G d ouble dagger = +0.34 kJ/mol). After formation of the alpha-agostic pi- complex the insertion proceeds without any large barriers directly to a beta-agostic product via a gamma-agostic primary product. The barrie r of insertion is 2.0 kJ/mol and barrier for the product reorientation amounts to 2.5 kJ/mol. The overall reaction is exothermic by -98.2 kJ /mol. The propagation barrier corresponds to the rearrangement prior t o insertion and rotation takes place in a concerted fashion. H-exchang e (chain termination) has a higher electronic barrier (Delta H double dagger = +28.2 kJ/mol), and an only slightly lower free energy of acti vation (Delta S double dagger = -4.5 J/(mol . K); Delta G double dagge r = +24.2 kJ/mol). Rotation is favored over H-exchange because of the high flexibility of the pi-complex. This gives a ratio of 15000/1 (ins ertion/H-exchange) based on Maxwell-Boltzmann statistics. Backside ins ertion starts with the formation of a backside pi-complex and has an a ctivation barrier of 28.4 kJ/mol (Delta S double dagger: = -16.1 J/(mo l . K), Delta G double dagger = +32.5 kJ/mol).